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Journal of Russian Laser Research

Improved Wavelength Measurement of 2S1/2→2P1/2 and 2D3/2→3[3/2]1/2 Transitions in Yb+

Ilia V. Zalivako, Ilya A. Semerikov, Alexander S. Borisenko, Vasilii N. Smirnov, Pavel Vishnyakov, Mikhail A. Aksenov, Pavel Sidorov, N. Kolachevsky, Ksenia Yu. Khabarova

Published Jul 1, 2019• 12 citations
Publisher
DOI
10.1007/s10946-019-09814-3

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The luminescence excitation spectra of the D1 resonance line of atoms K, Rb, and Cs in gas mixtures with CF4 are found to contain satellite transitions, which correspond to the transition of an atom to the states (n – 1)d 2D3/2,5/2 and (n + 1)s 2S1/2, where n = 4, 5, and 6 for K, Rb, and Cs, respectively, with the simultaneous excitation of CF4 molecule vibrations at the IR active mode frequency ν3 with a quantum energy of 1283 cm–1. These satellite transitions are A(ns 2S1/2) + CF4(ν3 = 0) + hν → A((n – 1)d 2D3/2,5/2) + CF4(ν3 = 1) and A(ns 2S1/2) + CF4(ν3 = 0) + hν → A((n + 1)s 2S1/2) + CF4(ν3 = 1), where A = K, Rb, and Cs. The appearance of an optical coupling between the upper and lower states of these asymptotically (at $${{R}_{{{\text{A}} - {\text{C}}{{{\text{F}}}_{4}}}}}$$ → ∞) forbidden transitions is shown to be caused by the interaction of the dipole moment of the ν3 = 1 ↔ ν3 = 0 vibrational transition in the CF4 molecule with the dipole moments of the electronic transitions np 2P1/2,3/2 ↔ (n – 1)d 2D3/2,5/2 and np 2P1/2,3/2 ↔ (n + 1)s 2S1/2 in an alkali metal atom; as a result of this interaction, the upper state of the satellite transition acquires admixtures of the A(np 2P1/2,3/2)CF4(ν3 = 0) resonance states.

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Abstract The isotopic shifts of the 5s 2S1/2–5p 2P1/2 cooling transition, the 5p 2P1/2–4d 2D3/2 pumping transition, and the 5s 2S1/2–4d 2D5/2 electroquadrupole transition are measured in monoisotopic clouds of strontium ions: 88Sr+, 86Sr+, and 84Sr+. To the best of our knowledge, the isotopic shift of the clock transition at 674 nm in 84Sr+ is measured for the first time and is found to be 1186.7(7.2) MHz. The obtained experimental data is used to construct a King diagram, which allows the field (F) and mass (K) shift constants to be estimated for the transition at a wavelength of 674 nm. The obtained results can be used to test atomic structure calculations, sympathetic cooling, and quantum algorithms.
The luminescence excitation spectra of the D1 resonance line of atoms K, Rb, and Cs in gas mixtures with CF4 are found to contain satellite transitions, which correspond to the transition of an atom to the states (n – 1)d 2D3/2,5/2 and (n + 1)s 2S1/2, where n = 4, 5, and 6 for K, Rb, and Cs, respectively, with the simultaneous excitation of CF4 molecule vibrations at the IR active mode frequency ν3 with a quantum energy of 1283 cm–1. These satellite transitions are A(ns 2S1/2) + CF4(ν3 = 0) + hν → A((n – 1)d 2D3/2,5/2) + CF4(ν3 = 1) and A(ns 2S1/2) + CF4(ν3 = 0) + hν → A((n + 1)s 2S1/2) + CF4(ν3 = 1), where A = K, Rb, and Cs. The appearance of an optical coupling between the upper and lower states of these asymptotically (at RA−CF4{{R}_{{{\text{A}} - {\text{C}}{{{\text{F}}}_{4}}}}}RA−CF4​​ → ∞) forbidden transitions is shown to be caused by the interaction of the dipole moment of the ν3 = 1 ↔ ν3 = 0 vibrational transition in the CF4 molecule with the dipole moments of the electronic transitions np 2P1/2,3/2 ↔ (n – 1)d 2D3/2,5/2 and np 2P1/2,3/2 ↔ (n + 1)s 2S1/2 in an alkali metal atom; as a result of this interaction, the upper state of the satellite transition acquires admixtures of the A(np 2P1/2,3/2)CF4(ν3 = 0) resonance states.